Fall 2019 - Problem 7

measure theory, Stone-Weierstrass

Let JRJ \subseteq \R be a compact interval, and let μ\mu be a finite Borel measure whose support lies in JJ. For zCJz \in \C \setminus J define

Fμ(z)=R1ztdμ(t).F_\mu\p{z} = \int_\R \frac{1}{z - t} \,\diff\mu\p{t}.

Prove that the mapping μFμ\mu \mapsto F_\mu is one-to-one.

Solution.

Let t0RJt_0 \in \R \setminus J and δ=d(t0,J)>0\delta = d\p{t_0, J} > 0, since JJ is compact. Thus, if tJt \in J, then

1zt=1(zt0)(tt0)=1tt011zt0tt0=n=01tt0(zt0tt0)n=n=0(zz0)n(tt0)n+1\begin{aligned} \frac{1}{z - t} &= \frac{1}{\p{z - t_0} - \p{t - t_0}} \\ &= -\frac{1}{t - t_0} \frac{1}{1 - \frac{z - t_0}{t - t_0}} \\ &= -\sum_{n=0}^\infty \frac{1}{t - t_0} \p{\frac{z - t_0}{t - t_0}}^n \\ &= -\sum_{n=0}^\infty \frac{\p{z - z_0}^n}{\p{t - t_0}^{n+1}} \end{aligned}

converges locally uniformly on zt0<δ\abs{z - t_0} < \delta. Hence,

Fμ(z)=Rn=0(zz0)n(tt0)n+1dμ(t)=n=0(R1(tt0)n+1dμ(t))(zz0)n.\begin{aligned} F_\mu\p{z} &= -\int_\R \sum_{n=0}^\infty \frac{\p{z - z_0}^n}{\p{t - t_0}^{n+1}} \,\diff\mu\p{t} \\ &= \sum_{n=0}^\infty \p{-\int_\R \frac{1}{\p{t - t_0}^{n+1}} \,\diff\mu\p{t}} \p{z - z_0}^n. \end{aligned}

Hence, if Fμ=FνF_\mu = F_\nu, then by uniqueness of power series, we get

R1(tt0)n+1dμ(t)=R1(tt0)n+1dν(t)\int_\R \frac{1}{\p{t - t_0}^{n+1}} \,\diff\mu\p{t} = \int_\R \frac{1}{\p{t - t_0}^{n+1}} \,\diff\nu\p{t}

for all n0n \geq 0. Let

A={k=1Nck(tt0)nk|NN, ckR, nkN}.A = \set{\sum_{k=1}^N \frac{c_k}{\p{t - t_0}^{n_k}} \st N \in \N,\ c_k \in \R,\ n_k \in \N}.

This is a subalgebra which separates points and vanishes nowhere on JJ, so by Stone-Weierstrass, AA is dense in C(J)C\p{J}. Hence, μ=ν\mu = \nu on a dense subset of C(J)C\p{J}, so they agree on all of C(J)C\p{J}. By Riesz representation, this means μ=ν\mu = \nu as measures on JJ. Since μ\mu and ν\nu are supported on JJ, we see that μ=ν\mu = \nu as measures on R\R, which was what we wanted to show.